Methods of making a radiation detector

ABSTRACT

Disclosed herein is a method for forming a radiation detector. The method comprises forming a radiation absorption layer and bonding an electronics layer to the radiation absorption layer. The electronics layer comprises an electronic system configured to process electrical signals generated in the radiation absorption layer upon absorbing radiation photons. The method for forming the radiation absorption layer comprises forming a trench into a first surface of a semiconductor substrate; doping a sidewall of the trench; forming a first electrical contact on the first surface; forming a second electrical contact on a second surface of the semiconductor substrate. The second surface is opposite the first surface. The method further comprises dicing the semiconductor substrate along the trench.

TECHNICAL FIELD

The disclosure herein relates to methods of making a radiation detector,particularly relates to a method of forming a radiation detector with anactive edge.

BACKGROUND

A radiation detector is a device that measures a property of aradiation. Examples of the property may include a spatial distributionof the intensity, phase, and polarization of the radiation. Theradiation may be one that has interacted with a subject. For example,the radiation measured by the radiation detector may be a radiation thathas penetrated or reflected from the subject. The radiation may be anelectromagnetic radiation such as infrared light, visible light,ultraviolet light, X-ray or γ-ray. The radiation may be of other typessuch as α-rays and β-rays.

One type of radiation detectors is based on interaction between theradiation and a semiconductor. For example, a radiation detector of thistype may have a semiconductor layer that absorbs the radiation andgenerate charge carriers (e.g., electrons and holes) and circuitry fordetecting the charge carriers.

SUMMARY

Disclosed herein is a method comprising: forming a trench into a firstsurface of a semiconductor substrate; doping a sidewall of the trench;forming a first electrical contact on the first surface; forming asecond electrical contact on a second surface of the semiconductorsubstrate, the second surface being opposite the first surface.

According to an embodiment, the semiconductor substrate comprisessilicon, germanium, GaAs, CdTe, CdZnTe, or a combination thereof.

According to an embodiment, the trench extends through an entirethickness of the semiconductor substrate.

According to an embodiment, forming the trench comprises forming a maskon the first surface and etching portions of the semiconductor substrateuncovered by the mask.

According to an embodiment, the mask comprises silicon dioxide.

According to an embodiment, forming the trench comprises deepreactive-ion etching.

According to an embodiment, the method further comprises smoothening thesidewall by wet etching.

According to an embodiment, doping the sidewall comprises diffusinggaseous dopant into the sidewall.

According to an embodiment, doping the sidewall comprises depositingpolysilicon into the trench.

According to an embodiment, the method further comprises doping thepolysilicon after depositing the polysilicon.

According to an embodiment, doping the sidewall comprises annealing thesemiconductor substrate.

According to an embodiment, the second electrical contact comprisesdiscrete portions.

According to an embodiment, the method further comprises forming a diodein the semiconductor substrate by forming a first doped region into thefirst surface and a second doped region into the second surface.

According to an embodiment, the second doped region comprises discreteregions.

According to an embodiment, the first doped region and the sidewall havea same type of doping.

According to an embodiment, the second doped region and the first dopedregion have opposite types of doping.

According to an embodiment, the method further comprises dicing thesemiconductor substrate along the trench.

According to an embodiment, the method further comprises bonding thesemiconductor substrate to another substrate comprising an electronicsystem therein or thereon.

According to an embodiment, the electronic system comprises a voltagecomparator configured to compare a voltage of the second electricalcontact to a first threshold; a counter configured to register a numberof photons of radiation absorbed by the radiation absorption layer; acontroller; a voltmeter; wherein the controller is configured to start atime delay from a time at which the voltage comparator determines thatan absolute value of the voltage equals or exceeds an absolute value ofthe first threshold; wherein the controller is configured to cause thevoltmeter to measure the voltage upon expiration of the time delay;wherein the controller is configured to determine a number of photons bydividing the voltage measured by the voltmeter by a voltage that asingle photon would have caused on the second electrical contact;wherein the controller is configured to cause the number registered bythe counter to increase by the number of photons.

According to an embodiment, the electronic system further comprising acapacitor module electrically connected to the second electricalcontact, wherein the capacitor module is configured to collect chargecarriers from the second electrical contact.

According to an embodiment, the controller is configured to connect thesecond electrical contact to an electrical ground.

According to an embodiment, the controller is configured to deactivatethe voltage comparator at a beginning of the time delay.

Disclosed herein is a detector comprising: a radiation absorption layercomprising a first surface, a first electrical contact on the firstsurface, a second surface opposite the first surface, a secondelectrical contact on the second surface, and a sidewall; wherein thesidewall is doped; an electronics layer bonded to the radiationabsorption layer, the electronics layer comprising electronic systemconfigured to process electrical signals on the second electricalcontact.

According to an embodiment, the radiation absorption layer comprisessilicon, germanium, GaAs, CdTe, CdZnTe, or a combination thereof.

According to an embodiment, the second electrical contact comprisesdiscrete portions.

According to an embodiment, the sidewall is the only doped sidewall ofthe radiation absorption layer.

According to an embodiment, the radiation absorption layer comprises adiode comprising a first doped region and a second doped region, whereinthe first doped region and the second doped region are in the firstsurface and the second surface respectively.

According to an embodiment, the second doped region comprises discreteregions.

According to an embodiment, the first doped region and the sidewall havea same type of doping.

According to an embodiment, the first doped region and the second dopedregion have opposite types of doping.

According to an embodiment, the electronic system comprises a voltagecomparator configured to compare a voltage of the second electricalcontact to a first threshold; a counter configured to register a numberof photons of radiation absorbed by the semiconductor substrate; acontroller; a voltmeter; wherein the controller is configured to start atime delay from a time at which the voltage comparator determines thatan absolute value of the voltage equals or exceeds an absolute value ofthe first threshold; wherein the controller is configured to cause thevoltmeter to measure the voltage upon expiration of the time delay;wherein the controller is configured to determine a number of photons bydividing the voltage measured by the voltmeter by a voltage that asingle photon would have caused on the second electrical contact;wherein the controller is configured to cause the number registered bythe counter to increase by the number of photons.

According to an embodiment, the electronic system further comprising acapacitor module electrically connected to the second electricalcontact, wherein the capacitor module is configured to collect chargecarriers from the second electrical contact.

According to an embodiment, the controller is configured to connect thesecond electrical contact to an electrical ground.

According to an embodiment, the controller is configured to deactivatethe voltage comparator at a beginning of the time delay.

Disclosed herein is a system comprising: a first package comprising afirst radiation detector, the first radiation detector being theradiation detector of any one of the radiation detectors disclosedabove; wherein no sidewalls of the first radiation detector except thesidewall that is doped are configured to be exposed to radiationincident on the system.

According to an embodiment, the system further comprises a secondpackage comprising a second radiation detector, wherein the secondpackage is configured to prevent radiation from reaching a sidewall ofthe first radiation detector that is not doped.

According to an embodiment, the first package is mounted to a system PCBand the first radiation detector is tilted relative to the system PCB.

BRIEF DESCRIPTION OF FIGURES

FIG. 1 schematically shows a radiation detector, according to anembodiment.

FIG. 2A schematically shows a cross-sectional view of the radiationdetector, according to an embodiment.

FIG. 2B schematically shows a detailed cross-sectional view of theradiation detector in FIG. 2A, according to an embodiment.

FIG. 2C schematically shows an alternative detailed cross-sectional viewof the radiation detector in FIG. 2A, according to an embodiment.

FIG. 2D schematically illustrates a top view of the radiation detectorin FIG. 2A, according to an embodiment.

FIG. 3 schematically illustrates a process of forming the radiationabsorption layer in FIG. 2B, which includes diodes, according to anembodiment.

FIG. 4 schematically illustrates a process of forming the radiationabsorption layer in FIG. 2C, which includes resistors not diodes,according to an embodiment.

FIG. 5 schematically illustrates bonding between the radiationabsorption layer and the electronics layer to form the radiationdetector in FIG. 2A, according an embodiment.

FIG. 6A schematically shows a top view of a package including aradiation detector and a printed circuit board (PCB), according to anembodiment.

FIG. 6B and FIG. 6C schematically show a top view and a cross-sectionalview of a system comprising a plurality of the packages, according to anembodiment.

FIG. 7A and FIG. 7B each show a component diagram of the electronicsystem, according to an embodiment.

FIG. 8 schematically shows a temporal change of the voltage of theelectrode or the electrical contact, according to an embodiment.

DETAILED DESCRIPTION

FIG. 1 schematically shows a radiation detector 100, as an example. Theradiation detector 100 has an array of pixels 150. The array may be arectangular array, a honeycomb array, a hexagonal array or any othersuitable array. Each pixel 150 is configured to detect radiation from aradiation source incident thereon and may be configured measure acharacteristic (e.g., the energy of the particles, the wavelength, andthe frequency) of the radiation. For example, each pixel 150 isconfigured to count numbers of photons incident thereon whose energyfalls in a plurality of bins, within a period of time. All the pixels150 may be configured to count the numbers of photons incident thereonwithin a plurality of bins of energy within the same period of time.When the incident photons have similar energy, the pixels 150 may besimply configured to count numbers of photons incident thereon within aperiod of time, without measuring the energy of the individual photons.Each pixel 150 may have its own analog-to-digital converter (ADC)configured to digitize an analog signal representing the energy of anincident photon into a digital signal, or to digitize an analog signalrepresenting the total energy of a plurality of incident photons into adigital signal. The pixels 150 may be configured to operate in parallel.For example, when one pixel 150 measures an incident photon, anotherpixel 150 may be waiting for a photon to arrive. The pixels 150 may nothave to be individually addressable.

FIG. 2A schematically shows a cross-sectional view of the radiationdetector 100, according to an embodiment. The radiation detector 100 mayinclude a radiation absorption layer 110 configured to absorb anincident radiation and generate electrical signals from incidentradiation, and an electronics layer 120 (e.g., an ASIC) for processingor analyzing the electrical signals generates in the radiationabsorption layer 110. The radiation detector 100 may or may not includea scintillator. The radiation absorption layer 110 may include asemiconductor material such as, silicon, germanium, GaAs, CdTe, CdZnTe,or a combination thereof. The semiconductor may have a high massattenuation coefficient for the radiation of interest.

FIG. 2B schematically shows a detailed cross-sectional view of theradiation detector 100, according to an embodiment. The radiationabsorption layer 110 may comprise a first doped region 111 formed bydoping a first surface 101, a second doped region 113 formed by doping asecond surface 102, and a doped sidewall 116. The second surface 102 isopposite the first surface 101. The second doped region 113 may compriseone or more discrete regions 114. The radiation absorption layer 110 mayfurther comprise a first electrical contact 119A on the first surface101, a second electrical contact 119B on the second surface 102. Thefirst electrical contact 119A may be in electrical contact with thefirst doped region 111 and the doped sidewall 116. The second electricalcontact 119B may include discrete portions each of which is inelectrical contact with the discrete regions 114. The doped sidewall 116may be at all sides of the radiation absorption layer 110.

The doped sidewall 116 has a same type of doping as the first dopedregion 111 (e.g., both the first doped region 111 and the doped sidewall116 are p type, or both the first doped region 111 and the dopedsidewall 116 are n type). The doped sidewall 116 can be joined with thefirst doped region 111 and thus viewed as an extension thereof. Thesecond doped region 113 may be separated from the first doped region 111and the doped sidewall 116 by an optional the intrinsic region 112. Thediscrete regions 114 are separated from one another by the first dopedregion 111 or the intrinsic region 112. The first doped region 111 andthe second doped region 113 have opposite types of doping (e.g., region111 is p-type and region 113 is n-type, or region 111 is n-type andregion 113 is p-type).

One or more diodes (e.g., p-i-n or p-n) may be formed by the first dopedregion 111 and the one or more discrete regions 114 of the second dopedregion 113. The first doped region 111 and the doped sidewall 116 maycollectively be an electrode shared among the diodes, and each of thediscrete regions 114 of the second doped region 113 may be anotherelectrode of the diodes. The first doped region 111 may also havediscrete portions.

When radiation from the radiation source hits the radiation absorptionlayer 110 including diodes, the radiation photon may be absorbed andgenerate one or more charge carriers by a number of mechanisms. Thecharge carriers may drift to the electrodes (e.g., the first dopedregion 111, the discrete regions 114) of one of the diodes under anelectric field. The field may be an external electric field applied tothe first and second electrical contacts 119A and 119B. In anembodiment, the charge carriers may drift in directions such that thecharge carriers generated by a single particle of the radiation are notsubstantially shared by two different discrete regions 114 (“notsubstantially shared” here means less than 2%, less than 0.5%, less than0.1%, or less than 0.01% of these charge carriers flow to a differentone of the discrete regions 114 than the rest of the charge carriers).Charge carriers generated by a particle of the radiation incident aroundthe footprint of one of these discrete regions 114 are not substantiallyshared with another of these discrete regions 114. A pixel 150associated with a discrete region 114 may be an area around the discreteregion 114 in which substantially all (more than 98%, more than 99.5%,more than 99.9%, or more than 99.99% of) charge carriers generated by aparticle of the radiation incident therein flow to the discrete region114. Namely, less than 2%, less than 1%, less than 0.1%, or less than0.01% of these charge carriers flow beyond the pixel.

As shown in an alternative detailed cross-sectional view of theradiation detector 100 in FIG. 2C, according to an embodiment, theradiation absorption layer 110 may include a resistor of a semiconductormaterial such as, silicon, germanium, GaAs, CdTe, CdZnTe, or acombination thereof, but does not include a diode. The semiconductor mayhave a high mass attenuation coefficient for the radiation of interest.

When the radiation hits the radiation absorption layer 110 including aresistor but not diodes, it may be absorbed and generate one or morecharge carriers by a number of mechanisms. A particle of the radiationmay generate 10 to 100000 charge carriers. The charge carriers may driftto the first and second electrical contacts 119A and 119B under anelectric field. The field may be an external electric field. The secondelectrical contact 119B includes discrete portions. In an embodiment,the charge carriers may drift in directions such that the chargecarriers generated by a single particle of the radiation are notsubstantially shared by two different discrete portions of the secondelectrical contact 119B (“not substantially shared” here means less than2%, less than 0.5%, less than 0.1%, or less than 0.01% of these chargecarriers flow to a different one of the discrete portions than the restof the charge carriers). Charge carriers generated by a particle of theradiation incident around the footprint of one of these discreteportions of the second electrical contact 119B are not substantiallyshared with another of these discrete portions of the electrical contact119B. A pixel 150 associated with a discrete portion of the secondelectrical contact 119B may be an area around the discrete portion inwhich substantially all (more than 98%, more than 99.5%, more than 99.9%or more than 99.99% of) charge carriers generated by a particle of theradiation incident therein flow to the discrete portion of the secondelectrical contact 119B. Namely, less than 2%, less than 0.5%, less than0.1%, or less than 0.01% of these charge carriers flow beyond the pixelassociated with the one discrete portion of the second electricalcontact 119B. The doped sidewall 116 may help prevent current leakage atthe sidewall.

FIG. 2D schematically illustrates a top view of the radiation detector100, according to an embodiment. The radiation detector 100 may have arectangular shape, a hexagonal shape or any other suitable shapes. Theradiation detector 100 may have one or more doped sidewalls. In exampleof FIG. 2D, the radiation detector 100 has a rectangular shape, and thedoped sidewall 116 is the only doped sidewall of the radiationabsorption layer 110. The doped sidewall 116 and the discrete regions(e.g., 114 or 119B) in FIG. 2D are shown in dashed line since theycannot be seen directly from the top view.

The electronics layer 120 may include an electronic system 121configured to process electrical signals on the second electricalcontact 119B generated by the radiation incident on the radiationabsorption layer 110. The electronic system 121 may include an analogcircuitry such as a filter network, amplifiers, integrators, andcomparators, or a digital circuitry such as a microprocessors, andmemory. The electronic system 121 may include one or more ADCs. Theelectronic system 121 may include components shared by the pixels orcomponents dedicated to a single pixel. For example, the electronicsystem 121 may include an amplifier dedicated to each pixel and amicroprocessor shared among all the pixels. The electronic system 121may be electrically connected to the pixels by vias 131. Space among thevias may be filled with a filler material 130, which may increase themechanical stability of the connection of the electronics layer 120 tothe radiation absorption layer 110. Other bonding techniques arepossible to connect the electronic system 121 to the pixels withoutusing vias.

FIG. 3 schematically illustrates a process of forming the radiationabsorption layer 110 in FIG. 2B, which includes diodes, according to anembodiment.

In step 1000, a mask layer 204 is formed onto a first surface 201 of asubstrate 200. The substrate 200 may be attached to a support 206. Thesubstrate 200 may include a semiconductor material such as, silicon,germanium, GaAs, CdTe, CdZnTe, or a combination thereof. The mask layer204 may serve as an etch mask for forming trenches 208 as shown in step1002. The mask layer 204 may comprise a material such as silicondioxide, silicon nitride, amorphous carbon or metals (e.g., aluminum,chromium). The thickness of the mask layer 204 may be determinedaccording to the depth of the trenches 208 and etching selectivity(i.e., ratio of etching rates of the mask layer 204 and the substrate200). In an embodiment, the mask layer 204 may have a thickness of a fewmicrons. The mask layer 204 may be formed onto the first surface 201 byvarious techniques, such as physical vapor deposition, chemical vapordeposition, spin coating, sputtering or any other suitable processes. Inan embodiment, the substrate 200 is a silicon substrate, and the masklayer 204 is a silicon dioxide layer formed by thermal oxidation of thesurface of the substrate 200, where the substrate 200 is exposed tooxygen (“dry oxidation”) or a mixture of high-purity oxygen and hydrogen(“wet oxidation”) at an elevated temperature (e.g., 800-1200° C.) in afurnace, thereby causing the silicon on the surface of the substrate 200to react with oxygen in the environment to form the silicon dioxidelayer.

In step 1001, the mask layer 204 is patterned to have openings in whichthe substrate 200 is exposed. Shapes and locations of the openingscorrespond to the shapes and locations of the trenches 208 to form instep 1002. The pattern formation on the mask layer 204 may involvelithography process or any other suitable processes. For example, aresist layer may be first deposited (e.g., by spin coating) onto thesurface of the mask layer 204, and lithography is followed to form theopenings. The resolution of the lithography is limited by the wavelengthof the radiation used. Photolithography tools using deep ultraviolet(DUV) light with wavelengths of approximately 248 and 193 nm, allowsminimum feature sizes down to about 50 nm. E-beam lithography toolsusing electron energy of 1 keV to 50 keV allows minimum feature sizesdown to a few nanometers.

In step 1002, the trenches 208 are formed into the first surface 201 ofthe substrate 200 by etching portions of the substrate 200 uncovered bythe mask layer 204 to a desired depth (e.g., the trenches 208 may extendthrough an entire thickness of the substrate 200). The trenches 208 maybe vertical to the first surface 201. The etching process may be carriedout a technique such as dry etching, wet etching, or a combinationthereof. Dry etching is a type of etching processes such as ion beametching, plasma etching, reactive-ion etching, deep reactive-ion etching(DRIE), etc. Areas not protected by a mask (e.g., photoresist mask orother types of masks) may be removed physically or chemically with a dryetching process. Wet etching is a type of etching processes usingliquid-phase etchants. A substrate may be immersed in a bath of etchant,and areas not protected by the masks may be removed.

In an embodiment, forming the trenches 208 may comprise deepreactive-ion etching (DRIE). DRIE is capable of producing deeppenetration, steep-sided holes and highly vertical trenches insubstrates. The depth of the trenches 208 may be controlledapproximately by adjusting etching time and etch rate of the DRIE. Thesidewalls of the trenches 208 excavated with DRIE may have roughsurfaces. For example, during a Bosch process (which is one type ofDRIE), substrate materials are incrementally excavated with tworepeatedly alternating processes (an isotropic plasma etching and adeposition of a chemically inert passivation layer), causing the sidewalls the trenches 208 to undulate with an amplitude of hundreds ofnanometer.

In step 1003, a wet etching may be carried out after the trenches 208are formed to smooth out the roughness of the sidewalls of the trenches208.

In step 1004, the mask layer 204 may be removed by wet etching, chemicalmechanical polishing or some other suitable techniques. In an embodimentwhere the mask layer 204 is a silicon dioxide layer, the mask layer 204can be removed by hydrofluoric acid (HF) or buffered HF. Hydrofluoricacid essentially does not etch silicon.

The sidewalls of the trenches 208 and the first surface 201 may be dopedby various methods, such as a first doping method illustrated in steps1005 a-1005 c, or a second doping method illustrated in steps 1006a-1006 b. Each of the doped sidewalls 216 (as shown in 1005 b, 1005 c,1006 a and 1006 b) of the trenches 208 may function as the dopedsidewall 116 of the radiation absorption layer 110. Doping the firstsurface 201 forms a first doped region 211 (as shown in 1005 b, 1005 c,1006 a and 1006 b). A portion of the first doped region 211 may functionas the first doped region 111 of the radiation absorption layer 110.

In the first doping method illustrated in steps 1005 a-1005 c, dopingthe sidewalls of the trenches 208 and the first surface 201 comprisesdepositing doped polysilicon 205 or other suitable materials into thetrenches 208 and onto the first surface 201, as shown in step 1005 a. Inan embodiment, forming the doped polysilicon 205 may involve an in-situdoping technique, in which the polysilicon doping is carried out duringthe polysilicon deposition process. A chemical vaporization deposition(CVD) process may be used to deposited polysilicon at elevatedtemperature (e.g., around 600° C.), and the p type or n type dopantgases (e.g., phosphine, arsine, or diborane) are added to the reactantgases (e.g., silane) used for polysilicon deposition with CVD. Inanother embodiment, the polysilicon deposition may be carried out first,and then the polysilicon is doped. The p type or n type dopants may bedeposited into the polysilicon by methods such as diffusion doping andion implantation. For instance, p type or n type dopants may bedeposited into the polysilicon region by directly bombarding the regionwith high-energy ions of the dopant species.

In step 1005 b, the substrate 200 is annealed. The dopants in the dopedpolysilicon 205 diffuse into the first surface 201 and the sidewalls ofthe trenches 208 at elevated temperatures (e.g., around 900° C.), sothat the first doped region 211 and the doped sidewalls 216 form. Thehigh-temperature environment of the annealing not only promotes dopantdiffusion from doped polysilicon 205, but also anneals out defects ofthe first doped region 211, the doped sidewalls 216 and the substrate200.

In step 1005 c, the doped polysilicon 205 on top of the first surface201 may be removed by a method such as wet etching, chemical mechanicalpolishing or any other suitable techniques. Meanwhile, the dopedpolysilicon 205 in the trenches 208 are retained to provide a levelsurface for following steps such as depositing electrical contacts.

In the second doping method illustrated in step 1006 a and step 1006 b,which is an alternative to the first doping method illustrated in steps1005 a-1005 c, doping the sidewalls of the trenches 208 and the firstsurface 201 comprises diffusing gaseous dopants into the sidewalls ofthe trenches 208 and the first surface 201, as shown in step 1006 a. Acarrier gas (e.g., nitrogen, argon) enriched with the desired dopant maybe led to the first surface 201 and the sidewalls of the trenches 208.The dopants gradually diffuse into the substrate 200 so that the firstdoped region 211 and the doped sidewalls 216 form. The substrate 200 maybe annealed during or after diffusion to drive the dopants deeper intothe substrate 200.

In step 1006 b, the trenches 208 may be filled with a filler material207 to provide a level surface for following steps such as depositingelectrical contacts. The filler material 207 may be polysilicon or anyother suitable materials.

In an embodiment, doping the sidewalls of the trenches 208 and the firstsurface 201 are not necessarily done at the same time or in a sameprocess as shown in step 1005 a-step 1005 c or step 1006 a-step 1006 b.For example, the sidewalls of the trenches 208 can be doped right afterstep 1003 before removing the mask layer 204 and doping the firstsurface 201.

In step 1007, a second doped region 213 is formed by doping a secondsurface 202 of the substrate 200. The second surface 202 is opposite thefirst surface 201. The substrate 200 may be lifted off from the support206 prior to the doping. The second doped region 213 and the first dopedregion 211 are doped with opposite types of dopants (e.g., region 211 isp-type and region 213 is n-type, or region 211 is n-type and region 213is p-type). In an embodiment, the second doped region 213 may compriseone or more discrete regions 214 that are doped. A portion of the seconddoped region 213 may function as the second doped region 113 of theradiation absorption layer 110, and some of the discrete regions 214 mayfunction as the discrete regions 114. Doping the discrete regions 214may involve a process similar to the step 1001, in which a mask withopenings is formed. Shapes and locations of the openings correspond tothe shapes and locations of the discrete regions 214. The discreteregions 214 uncovered by the mask are doped by a method such asdiffusion or ion implantation, and processes such as annealing and maskremoval may follow after doping.

In step 1008, the first and second electrical contacts 219A and 219B aredeposited onto the first surface 201 and the second surface 202respectively. The first and second electrical contacts 219A and 219Beach of which may comprise a conducting material such as a metal (e.g.,gold, copper, aluminum, platinum, etc.), or any other suitableconducting materials. A portion of the first electrical contact 219A mayfunction as the first electrical contact 119A of the radiationabsorption layer 110. A portion of the second electrical contact 219Bmay function as the second electrical contact 119B of the radiationabsorption layer 110 in FIG. 2B. The second electrical contact 219B maycomprise discrete regions each of which is in electrical contact withthe discrete regions 214.

Forming the first and second electrical contacts 219A and 219B mayinvolve forming masks with openings on the first and second surface 202respectively by processes similar to the step 1001 shown in FIG. 3.Conducing materials such as metal may be deposited into the openings theby a suitable technique such as physical vapor deposition, chemicalvapor deposition, spin coating, sputtering, etc., so that the first andsecond electrical contacts 219A and 219B form. The first and secondelectrical contacts 219A and 219B may not cover the top and bottomsurfaces of the filler material 207 in the trenches 208, which arecovered by the masks before the masks are removed.

In step 1009 and step 1010, one or more dies 230 are cut out bysubstrate dicing, which is followed by some post-dicing treatments. Eachof the one or more dies 230 is an embodiment of the radiation absorptionlayer 110. The first doped region 211, the discrete regions 214 of thesecond doped region 213, the doped sidewall 216 and the first and secondelectrical contacts 219A and 219B of the die 230 correspond to the firstdoped region 111, the discrete regions 114 of the second doped region113, the doped sidewall 116 and the first and second electrical contacts119A and 119B of the radiation absorption layer 110 respectively. In anembodiment, an interior region of the substrate 200 of the die 230 mayremain intrinsic and correspond to the intrinsic region 112 of theradiation absorption layer 110.

In step 1009, substrate dicing is performed by dicing along a pluralityof dicing streets 220 to separate the one or more dies 230 from eachother and from the rest of the substrate 200. The dicing streets 220 maycut through and section the trenches 208. The whole substrate may beattached to a support 206 during the substrate dicing. The substratedicing may involve processes such as dicing etching, mechanical sawingor laser cutting.

In step 1010, some post-dicing treatments may be performed, includingremoving the filler material 207, lifting off the dies 230 from thesupport 206, etc. Removing the filler material 207 may comprise anisotropic etching such as wet etching.

Forming the radiation absorption layer 110 may comprise someintermediate steps such as surface cleaning, polishing, surfacepassivation, which are not shown in FIG. 3. The order of the steps shownin FIG. 3 may be changed to suit different formation needs. For example,the second doped region 213 may be doped before the first doped region211.

FIG. 4 schematically illustrates a process of forming the radiationabsorption layer 110 as shown in FIG. 2C, which includes resistors notdiodes, according to an embodiment.

In step 2000, a semiconductor substrate shown in step 1003 of FIG. 3 isacquired, by carrying out steps 1000-1003 of FIG. 3. In an embodiment,the mask layer (i.e., 204 in steps 1000-1003) formed onto the firstsurface 201 comprises a conducting material such as metals (e.g.aluminum, copper, gold, platinum, etc.), so that the mask layer also mayfunction as the first electrical contact 219A.

In step 2001, the sidewalls of the trenches 208 are doped and becomedoped sidewalls 216, by either the first method illustrated in steps1005 a-1005 c or the second method illustrated in step 1006 a and step1006 b. Since the first surface in step 2001 is covered by the firstelectrical contact 219A, the first surface 201 is not doped during thedoping of the sidewalls. The trenches 208 are filled with a fillermaterial 207 to provide level surface for following steps such asdepositing electrical contacts. The filler material 207 may bepolysilicon (e.g., 205 in step 1005 c) or any other suitable materials.

In step 2002, the second electrical contact 219B is deposited onto thesecond surface 202 by a process described in step 1008 of FIG. 3.

In step 2003, processes such as substrate dicing, filler material 207removal and die lifting are carried out by following the steps 1009-1010described in FIG. 3. Each of the one or more dies 230 in FIG. 4 is anembodiment of the radiation absorption layer 110 in FIG. 2C, whichincludes resistors not diodes. The doped sidewall 216 and the first andsecond electrical contacts 219A and 219B of the die 230 correspond tothe doped sidewall 116 and the first and second electrical contacts 119Aand 119B of the radiation absorption layer 110 in FIG. 2C respectively.

FIG. 5 schematically illustrates bonding between the radiationabsorption layer 110 and the electronics layer 120 to form the radiationdetector 100, according an embodiment. Each of the discrete regions ofthe second electrical contact 119B may bond to each of the vias 131 by asuitable technique such as direct bonding or flip chip bonding.

Direct bonding is a wafer bonding process without any additionalintermediate layers (e.g., solder bumps). The bonding process is basedon chemical bonds between two surfaces. Direct bonding may be atelevated temperature but not necessarily so.

Flip chip bonding uses solder bumps 132 deposited onto contact pads(e.g., discrete regions of the second electrical contact 119B of theradiation absorption layer 110 or contacting surfaces of the vias 131).Either the radiation absorption layer 110 or the electronic layer 120 isflipped over and discrete regions of the second electrical contact 119Bare aligned to the vias 131. The solder bumps 132 may be melted tosolder the second electrical contact 119B and the vias 131 together. Anyvoid space among the solder bumps 199 may be filled with an insulatingmaterial.

FIG. 6A schematically shows a top view of a package 500 including aradiation detector 400 and a printed circuit board (PCB) 520, accordingto an embodiment. The radiation detector 400 is an embodiment of theradiation detector 100. The term “PCB” as used herein is not limited toa particular material. For example, a PCB may include a semiconductor.The radiation detector 400 is mounted to the PCB 520. The wiring betweenthe radiation detector 400 and the PCB 520 is not shown for the sake ofclarity. The electrical connection between the PCBs 520 in the packages500 and a system PCB (e.g., system PCB 550 in FIG. 6B and 6C) are madeby bonding wires 510. The radiation detector 400 may have an active area490, which is where the radiation detection occurs. The radiationdetector 400 may comprise a doped sidewall 416, and no sidewalls of theradiation detector 400 except the doped sidewall 416 are configured tobe exposed to radiation incident on the package 500. The PCB 520 maycomprise an area 505 that is not covered by the radiation detector 400,for accommodating bonding wires 510. The area 505 may be considered tobe part of a dead zone of the package 500, in which incident photonscannot be detected.

FIG. 6B and FIG. 6C schematically show a top view and a cross-sectionalview of a system comprising a plurality of the packages 500, accordingto an embodiment. The system may be an image sensor. The packages 500may be mounted to a system PCB 550 and are arranged in a row. Thepackages 500 may be tilted relative to the system 550 as shown in FIG.6C. The packages 500 in a row partially overlap with one another(analogous to a column of roofing shingles) as shown in FIG. 6B and FIG.6C, such that, within a row, one un-doped sidewall of the radiationdetector 400 and the area 505 of a package 500 are shadowed by itsneighboring package to prevent radiation from reaching the un-dopedsidewall and the area 505 of the package 500. The other un-dopedsidewalls of the radiation detector 400 may also be covered so thatradiation will not reach the other un-doped sidewalls of the radiationdetector 400.

FIG. 7A and FIG. 7B each show a component diagram of the electronicsystem 121, according to an embodiment. The electronic system 121 mayinclude a first voltage comparator 301, a second voltage comparator 302,a counter 320, a switch 305, a voltmeter 306 and a controller 310.

The first voltage comparator 301 is configured to compare the voltage ofan electrode of a diode to a first threshold. The diode may be a diodeformed by the first doped region 111, one of the discrete regions 114 ofthe second doped region 113, and the optional intrinsic region 112.Alternatively, the first voltage comparator 301 is configured to comparethe voltage of an electrical contact (e.g., a discrete portion ofelectrical contact 119B) to a first threshold. The first voltagecomparator 301 may be configured to monitor the voltage directly, orcalculate the voltage by integrating an electric current flowing throughthe diode or electrical contact over a period of time. The first voltagecomparator 301 may be controllably activated or deactivated by thecontroller 310. The first voltage comparator 301 may be a continuouscomparator. Namely, the first voltage comparator 301 may be configuredto be activated continuously, and monitor the voltage continuously. Thefirst voltage comparator 301 configured as a continuous comparatorreduces the chance that the electronic system 121 misses signalsgenerated by an incident radiation photon. The first voltage comparator301 configured as a continuous comparator is especially suitable whenthe incident radiation intensity is relatively high. The first voltagecomparator 301 may be a clocked comparator, which has the benefit oflower power consumption. The first voltage comparator 301 configured asa clocked comparator may cause the electronic system 121 to miss signalsgenerated by some incident radiation photons. When the incidentradiation intensity is low, the chance of missing an incident radiationphoton is low because the time interval between two successive photonsis relatively long. Therefore, the first voltage comparator 301configured as a clocked comparator is especially suitable when theincident radiation intensity is relatively low. The first threshold maybe 5-10%, 10%-20%, 20-30%, 30-40% or 40-50% of the maximum voltage oneincident radiation photon may generate in the diode or the resistor. Themaximum voltage may depend on the energy of the incident radiationphoton (i.e., the wavelength of the incident radiation), the material ofthe radiation absorption layer 110, and other factors. For example, thefirst threshold may be 50 mV, 100 mV, 150 mV, or 200 mV.

The second voltage comparator 302 is configured to compare the voltageto a second threshold. The second voltage comparator 302 may beconfigured to monitor the voltage directly, or calculate the voltage byintegrating an electric current flowing through the diode or theelectrical contact over a period of time. The second voltage comparator302 may be a continuous comparator. The second voltage comparator 302may be controllably activate or deactivated by the controller 310. Whenthe second voltage comparator 302 is deactivated, the power consumptionof the second voltage comparator 302 may be less than 1%, less than 5%,less than 10% or less than 20% of the power consumption when the secondvoltage comparator 302 is activated. The absolute value of the secondthreshold is greater than the absolute value of the first threshold. Asused herein, the term “absolute value” or “modulus” |x| of a real numberx is the non-negative value of x without regard to its sign. Namely,

${x} = \left\{ {\begin{matrix}{x,{{{if}\mspace{14mu} x} \geq 0}} \\{{- x},{{{if}\mspace{14mu} x} \leq 0}}\end{matrix}.} \right.$

The second threshold may be 200%-300% of the first threshold. The secondthreshold may be at least 50% of the maximum voltage one incidentradiation photon may generate in the diode or resistor. For example, thesecond threshold may be 100 mV, 150 mV, 200 mV, 250 mV or 300 mV. Thesecond voltage comparator 302 and the first voltage comparator 310 maybe the same component. Namely, the system 121 may have one voltagecomparator that can compare a voltage with two different thresholds atdifferent times.

The first voltage comparator 301 or the second voltage comparator 302may include one or more op-amps or any other suitable circuitry. Thefirst voltage comparator 301 or the second voltage comparator 302 mayhave a high speed to allow the electronic system 121 to operate under ahigh flux of incident radiation. However, having a high speed is oftenat the cost of power consumption.

The counter 320 is configured to register a number of radiation photonsreaching the diode or resistor. The counter 320 may be a softwarecomponent (e.g., a number stored in a computer memory) or a hardwarecomponent (e.g., a 4017 IC and a 7490 IC).

The controller 310 may be a hardware component such as a microcontrollerand a microprocessor. The controller 310 is configured to start a timedelay from a time at which the first voltage comparator 301 determinesthat the absolute value of the voltage equals or exceeds the absolutevalue of the first threshold (e.g., the absolute value of the voltageincreases from below the absolute value of the first threshold to avalue equal to or above the absolute value of the first threshold). Theabsolute value is used here because the voltage may be negative orpositive, depending on whether the voltage of the cathode or the anodeof the diode or which electrical contact is used. The controller 310 maybe configured to keep deactivated the second voltage comparator 302, thecounter 320 and any other circuits the operation of the first voltagecomparator 301 does not require, before the time at which the firstvoltage comparator 301 determines that the absolute value of the voltageequals or exceeds the absolute value of the first threshold. The timedelay may expire before or after the voltage becomes stable, i.e., therate of change of the voltage is substantially zero. The phase “the rateof change of the voltage is substantially zero” means that temporalchange of the voltage is less than 0.1%/ns. The phase “the rate ofchange of the voltage is substantially non-zero” means that temporalchange of the voltage is at least 0.1%/ns.

The controller 310 may be configured to activate the second voltagecomparator during (including the beginning and the expiration) the timedelay. In an embodiment, the controller 310 is configured to activatethe second voltage comparator at the beginning of the time delay. Theterm “activate” means causing the component to enter an operationalstate (e.g., by sending a signal such as a voltage pulse or a logiclevel, by providing power, etc.). The term “deactivate” means causingthe component to enter a non-operational state (e.g., by sending asignal such as a voltage pulse or a logic level, by cut off power,etc.). The operational state may have higher power consumption (e.g., 10times higher, 100 times higher, 1000 times higher) than thenon-operational state. The controller 310 itself may be deactivateduntil the output of the first voltage comparator 301 activates thecontroller 310 when the absolute value of the voltage equals or exceedsthe absolute value of the first threshold.

The controller 310 may be configured to cause the number registered bythe counter 320 to increase by one, if, during the time delay, thesecond voltage comparator 302 determines that the absolute value of thevoltage equals or exceeds the absolute value of the second threshold.

The controller 310 may be configured to cause the voltmeter 306 tomeasure the voltage upon expiration of the time delay. The controller310 may be configured to connect the electrode to an electrical ground,so as to reset the voltage and discharge any charge carriers accumulatedon the electrode. In an embodiment, the electrode is connected to anelectrical ground after the expiration of the time delay. In anembodiment, the electrode is connected to an electrical ground for afinite reset time period. The controller 310 may connect the electrodeto the electrical ground by controlling the switch 305. The switch maybe a transistor such as a field-effect transistor (FET).

In an embodiment, the system 121 has no analog filter network (e.g., aRC network). In an embodiment, the system 121 has no analog circuitry.

The voltmeter 306 may feed the voltage it measures to the controller 310as an analog or digital signal.

The electronic system 121 may include a capacitor module 309electrically connected to the electrode of the diode or the electricalcontact, wherein the capacitor module is configured to collect chargecarriers from the electrode. The capacitor module can include acapacitor in the feedback path of an amplifier. The amplifier configuredas such is called a capacitive transimpedance amplifier (CTIA). CTIA hashigh dynamic range by keeping the amplifier from saturating and improvesthe signal-to-noise ratio by limiting the bandwidth in the signal path.Charge carriers from the electrode accumulate on the capacitor over aperiod of time (“integration period”) (e.g., as shown in FIG. 4, betweent₀ to t₁, or t₁-t₂). After the integration period has expired, thecapacitor voltage is sampled and then reset by a reset switch. Thecapacitor module can include a capacitor directly connected to theelectrode.

FIG. 8 schematically shows a temporal change of the electric currentflowing through the electrode (upper curve) caused by charge carriersgenerated by a radiation photon incident on the diode or the resistor,and a corresponding temporal change of the voltage of the electrode(lower curve). The voltage may be an integral of the electric currentwith respect to time. At time t₀, the radiation photon hits the diode orthe resistor, charge carriers start being generated in the diode or theresistor, electric current starts to flow through the electrode of thediode or the resistor, and the absolute value of the voltage of theelectrode or electrical contact starts to increase. At time t₁, thefirst voltage comparator 301 determines that the absolute value of thevoltage equals or exceeds the absolute value of the first threshold V1,and the controller 310 starts the time delay TD1 and the controller 310may deactivate the first voltage comparator 301 at the beginning of TD1.If the controller 310 is deactivated before t₁, the controller 310 isactivated at t₁. During TD1, the controller 310 activates the secondvoltage comparator 302. The term “during” a time delay as used heremeans the beginning and the expiration (i.e., the end) and any time inbetween. For example, the controller 310 may activate the second voltagecomparator 302 at the expiration of TD1. If during TD1, the secondvoltage comparator 302 determines that the absolute value of the voltageequals or exceeds the absolute value of the second threshold at time t₂,the controller 310 causes the number registered by the counter 320 toincrease by one. At time t_(e), all charge carriers generated by theradiation photon drift out of the radiation absorption layer 110. Attime t_(s) the time delay TD1 expires. In the example of FIG. 8, timet_(s) is after time t_(e); namely TD1 expires after all charge carriersgenerated by the radiation photon drift out of the radiation absorptionlayer 110. The rate of change of the voltage is thus substantially zeroat t_(s). The controller 310 may be configured to deactivate the secondvoltage comparator 302 at expiration of TD1 or at t₂, or any time inbetween.

The controller 310 may be configured to cause the voltmeter 306 tomeasure the voltage upon expiration of the time delay TD1. In anembodiment, the controller 310 causes the voltmeter 306 to measure thevoltage after the rate of change of the voltage becomes substantiallyzero after the expiration of the time delay TD1. The voltage at thismoment is proportional to the amount of charge carriers generated by aradiation photon, which relates to the energy of the radiation photon.The controller 310 may be configured to determine the energy of theradiation photon based on voltage the voltmeter 306 measures. One way todetermine the energy is by binning the voltage. The counter 320 may havea sub-counter for each bin. When the controller 310 determines that theenergy of the radiation photon falls in a bin, the controller 310 maycause the number registered in the sub-counter for that bin to increaseby one. Therefore, the electronic system 121 may be able to detect aradiation image and may be able to resolve radiation photon energies ofeach radiation photon.

After TD1 expires, the controller 310 connects the electrode to anelectric ground for a reset period RST to allow charge carriersaccumulated on the electrode to flow to the ground and reset thevoltage. After RST, the electronic system 121 is ready to detect anotherincident radiation photon. Implicitly, the rate of incident radiationphotons the electronic system 121 can handle in the example of FIG. 8 islimited by 1/(TD1+RST). If the first voltage comparator 301 has beendeactivated, the controller 310 can activate it at any time before RSTexpires. If the controller 310 has been deactivated, it may be activatedbefore RST expires.

While various aspects and embodiments have been disclosed herein, otheraspects and embodiments will be apparent to those skilled in the art.The various aspects and embodiments disclosed herein are for purposes ofillustration and are not intended to be limiting, with the true scopeand spirit being indicated by the following claims.

1. (canceled)
 2. (canceled)
 3. (canceled)
 4. (canceled)
 5. (canceled) 6.(canceled)
 7. (canceled)
 8. (canceled)
 9. (canceled)
 10. (canceled) 11.(canceled)
 12. (canceled)
 13. (canceled)
 14. (canceled)
 15. (canceled)16. (canceled)
 17. (canceled)
 18. (canceled)
 19. (canceled) 20.(canceled)
 21. (canceled)
 22. (canceled)
 23. A detector comprising: aradiation absorption layer comprising a first surface, a firstelectrical contact on the first surface, a second surface opposite thefirst surface, a second electrical contact on the second surface, and asidewall; wherein the sidewall is doped; an electronics layer bonded tothe radiation absorption layer, the electronics layer comprising anelectronic system configured to process electrical signals on the secondelectrical contact.
 24. (canceled)
 25. The detector of claim 23, whereinthe second electrical contact comprises discrete portions.
 26. Thedetector of claim 23, wherein the sidewall is the only doped sidewall ofthe radiation absorption layer.
 27. The detector of claim 23, whereinthe radiation absorption layer comprises a diode comprising a firstdoped region and a second doped region, wherein the first doped regionand the second doped region are in the first surface and the secondsurface respectively.
 28. The detector of claim 27, wherein the seconddoped region comprises discrete regions.
 29. The detector of claim 27,wherein the first doped region and the sidewall have a same type ofdoping.
 30. The detector of claim 27, wherein the first doped region andthe second doped region have opposite types of doping.
 31. The detectorof claim 23, wherein the electronic system comprises a voltagecomparator configured to compare a voltage of the second electricalcontact to a first threshold; a counter configured to register a numberof photons of radiation absorbed by the radiation absorption layer; acontroller; a voltmeter; wherein the controller is configured to start atime delay from a time at which the voltage comparator determines thatan absolute value of the voltage equals or exceeds an absolute value ofthe first threshold; wherein the controller is configured to cause thevoltmeter to measure the voltage upon expiration of the time delay;wherein the controller is configured to determine a number of photons bydividing the voltage measured by the voltmeter by a voltage that asingle photon would have caused on the second electrical contact;wherein the controller is configured to cause the number registered bythe counter to increase by the number of photons.
 32. (canceled) 33.(canceled)
 34. The detector of claim 31, wherein the controller isconfigured to deactivate the voltage comparator at a beginning of thetime delay.
 35. A system comprising: a first package comprising a firstradiation detector, the first radiation detector being the detector ofclaim 23; wherein no sidewalls of the first radiation detector exceptthe sidewall that is doped are configured to be exposed to radiationincident on the system.
 36. The system of claim 35, further comprising asecond package comprising a second radiation detector, wherein thesecond package is configured to prevent radiation from reaching asidewall of the first radiation detector that is not doped.
 37. Thesystem of claim 35, wherein the first package is mounted to a system PCBand the first radiation detector is tilted relative to the system PCB.